Home Expansion and adaptation of the M5B12O25(OH) structure type to incorporate di- and trivalent transition metal cations
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Expansion and adaptation of the M5B12O25(OH) structure type to incorporate di- and trivalent transition metal cations

  • Leonard C. Pasqualini ORCID logo , Martina Tribus and Hubert Huppertz ORCID logo EMAIL logo
Published/Copyright: January 12, 2024
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Abstract

Five transition metal borates were synthesized in a Walker-type module under high-pressure/high-temperature conditions of 8–9 GPa and 800–1200 °C. They all exhibit the same interpenetrating, anionic borate network B12O2616−, crystallizing in the space group I41/acd, and therefore show high similarities to the borates Ti5B12O26 and Ga5B12O25(OH). Cr5B12O25(OH) and V5B12O25(OH) are isotypic to Ga5B12O25(OH), whereas Mn5Mn0.83B12O26 and Fe5Fe0.14B12O24.3(OH)1.7 feature the partial occupation of an additional, cuboctahedral cavity in the structure. This is due to a partial reduction of the cations to the oxidation state +2, as presented with the novel compound Mn5MnB12O22(OH)4, which only features Mn2+ for charge compensation. These structures feature a twelvefold coordination of manganese and iron.

1 Introduction

The titanium borate Ti5B12O26 discovered by A. Haberer et al. in 2009 was the first representative of a structure class that features an anionic framework which consists of two interpenetrating, three-dimensional networks of corner sharing (BO4) tetrahedra crystallizing in the space group I41/acd [1]. Since then, an exchange of the mixed valent Ti3+ and Ti4+ cations with triel elements was reported, which led to the incorporation of hydrogen atoms for charge compensation and to the discovery of the structurally very similar substance class M5B12O25(OH) (M = Al3+, Ga3+ and In3+) [2], [3], [4]. The topologically identical anionic framework is also formed in the oxonitridophosphate Mg2CaP6O3N10, which in contrast to the aforementioned borates also has a cuboctahedral cavity formed by the anionic network filled with Ca2+ cations [5]. Among the borates, there is one example with the composition In5B12O25(OH):Eu3+ in which this cavity was doped with 2 mol% Eu3+ [2], but never filled in a stoichiometric fashion. Besides their common structures, these compounds also share their formation conditions, as all specimen were synthesized via high-pressure/high-temperature (HP/HT) experiments. This structure can be transformed into a modification with higher symmetry, crystallizing in the cubic space group Fm 3 m [4].

The two interpenetrating networks consist of relatively large Fundamental Building Blocks (FBBs), composed of four B3O9 dreier rings, which together form a B12O22O8/2 cluster. This cluster is connected to four other FBBs in a tetrahedral arrangement by sharing two common oxygen vertices each. Within these FBBs, a cavity is formed, which is cuboctahedrally surrounded by 12 oxygen atoms. The structure is built up by two of these tetrahedrally connected networks and is therefore related to the arrangement of the atoms in the Zintl phase NaTl [6]. In Figure 1 the construction of a B12O22O8/2 cluster from four FBBs and the arrangement of these clusters to form the interpenetrating network is depicted. The charge compensating cations reside between the two interpenetrating borate networks. They occur in the form of either two edge sharing octahedra, M2O10, or an isolated MO6 octahedron.

Figure 1: 
A cluster of four B3O9 dreier rings form a B12O22O8/2 FBB. Each unit cell contains eight of these clusters, which are arranged as two interpenetrating networks (blue and orange). The bonds branching off the FBB indicate the tetrahedral connection within the network.
Figure 1:

A cluster of four B3O9 dreier rings form a B12O22O8/2 FBB. Each unit cell contains eight of these clusters, which are arranged as two interpenetrating networks (blue and orange). The bonds branching off the FBB indicate the tetrahedral connection within the network.

Figure 2 shows the different coordination polyhedra of the cations. The edge sharing M12O10 octahedra are tetrahedrally surrounded by two FFBs of each network (a). The isolated M2O6 octahedra are octahedrally surrounded by three FBBs of each of the interpenetrating networks (b). Within every FBB, there is one cavity to contain the M3O12 cuboctahedron (c). In each unit cell there are 16 M12O10 units, eight M2O6 octahedra and eight M3O12 cuboctahedra.

Figure 2: 
Different metal polyhedra and the surrounding anionic borate network. The coordinating oxygen atoms stem from the depicted B12O22O8/2 clusters, as shown in (c) for the M3O12 cuboctahedron. Two or three clusters of both networks surround the edge-sharing M12O10 octahedra (a) and the isolated M2O6 octahedron (b), respectively.
Figure 2:

Different metal polyhedra and the surrounding anionic borate network. The coordinating oxygen atoms stem from the depicted B12O22O8/2 clusters, as shown in (c) for the M3O12 cuboctahedron. Two or three clusters of both networks surround the edge-sharing M12O10 octahedra (a) and the isolated M2O6 octahedron (b), respectively.

Despite the comparably complex bonding situation in the Ti5B12O26 structure type, it can also be described within the concept of closest packing of spheres: the FBBs build a cubic closest packing, which is tetrahedrally connected, thus forming two interpenetrating networks. All interstitial sites of this ccp arrangement are filled by either M2O6 octahedra (octahedral void) or two edge sharing M12O10 octahedra (tetrahedral void) as is shown in Figure 3.

Figure 3: 
Breakdown of the arrangement within the structure with basic concepts. The FBBs of Ti5B12O26 form a cubic closest packing (blue and orange). The tetrahedral voids are depicted in (a), the octahedral voids in (b). (c) shows all centers of the FBBs and all cations.
Figure 3:

Breakdown of the arrangement within the structure with basic concepts. The FBBs of Ti5B12O26 form a cubic closest packing (blue and orange). The tetrahedral voids are depicted in (a), the octahedral voids in (b). (c) shows all centers of the FBBs and all cations.

The Ti5B12O26 structure type is an interesting candidate as a model substance with highly tunable parameters for several reasons:

  1. Three crystallographically distinct cationic sites of different sizes.

  2. Ability to be protonated for charge balance.

  3. Flexibility concerning the cationic radius of the hosted metal ions and therefore changes in the volume of the unit cell, which contains the same anionic substructure (Al5B12O25(OH): V = 2.536 nm3, In5B12O25(OH): V = 3.018 nm3).

To test the limits of this structure type, we systematically conducted explorative syntheses. The aim of these investigations was to shed light on the influence of cations (i.e. their charge, size and electronic configuration) and of the anionic network on the crystal structure and the tolerance of specific cations towards changes in their environment. This is the first paper presenting a series of remarkable high-pressure borates, which is capable of hosting at least 16 different elements as cations within the same anionic borate network.

Herein, we report the successful synthesis and analysis of five new transition metal borates with the sum formulæ M5B12O25(OH) (M = V3+, Cr3+), Mn5MnB12O22(OH)4, Mn5Mn0.83B12O26, and Fe5Fe0.14B12O24.3(OH)1.7. It is the first structure type that can host either of the four elements vanadium, chromium, manganese or iron in the same anionic borate structure.

2 Experimental section

2.1 Synthesis

The used starting materials were H3BO3 (≥99.8 %, Carl Roth, Karlsruhe, Germany) and B2O3 (99.9 %, Strem Chemicals, Newburyport, MA, USA) as boron sources and one of the respective oxides (V2O5 (≥99.6 %, Merck, Darmstadt, Germany), Cr2O3 (99 %, Merck, Darmstadt Germany), MnO (99 %, Sigma Aldrich, St. Louis, MO, USA), Mn2O3 (99 %, Sigma Aldrich, St. Louis, MO, USA) or Fe2O3 (≥99 %, Sigma-Aldrich, St. Louis, MO, USA)). To reduce V2O5, a stoichiometric quantity of elemental B (95 %, Goodfellow, Huntingdon, GB) replaced an equal amount of B2O3. To receive Cr5B12O25(OH), some Cr2O3 was replaced by Cr(NO3)3·9 H2O (99 %, Sigma Aldrich, St. Louis, MO, USA), and only B2O3 was used as a boron source; with increasing amount of oxide, larger crystals were obtained, however, the amount of CrBO3 as a side product also increased. The starting materials were mixed in a stoichiometric fashion, thoroughly ground in an agate mortar and encapsulated in a Pt capsule and placed in an α-BN (Henze Boron Nitride Products AG) crucible with a fitting lid of the same material. All experiments were carried out in 18/11 assemblies and the syntheses were performed via HP/HT methods using a Walker-type multianvil module within a 1000 t hydraulic press (Max Voggenreiter GmbH). A two-step process consisting of six steel wedges and eight tungsten carbide cubes (Hawedia) as outer and inner anvils was used to build up the pressure. Further details concerning this kind of setup are described in the literature [7], [8], [9].

The pressure, at which the syntheses were carried out, was 9 GPa for all substances, except for the synthesis of V5B12O25(OH), where 8 GPa were sufficient. Pressure was built up in 240 min, followed by heating to the desired temperature within 10 min. For V5B12O25(OH) and Cr5B12O25(OH), the maximum temperature was 1000 °C. The maximum temperature of the reaction was held for 60 min, followed by a step-wise reduction to 900 °C and eventually 800 °C with 2 K min−1, with keeping the temperature constant for 60 min at 900 and 800 °C. The maximum temperature for Fe5Fe0.14B12O24.3(OH)1.7 and Mn5Mn0.83B12O26 was 800 °C. After 20 min at 800 °C, the temperature was decreased to 400 °C within 200 min. Mn5MnB12O22(OH)4 was heated to 1200 °C, with a lowering of the temperature to 800 °C in 200 min after 20 min holding time at maximum temperature. Afterwards, the reaction mixture was quenched to room temperature within a few minutes in all cases. Decompression to ambient conditions was performed within 720 min. The Pt capsules were cleaned before collecting the crystalline products. An overview of all syntheses is shown in Table 1.

Table 1:

Ratio of starting materials and maximum reaction conditions.

Ratio of reactants Max. conditions
Substance Metal source M x O y B B2O3 H3BO3 p (GPa) T (°C)
V5B12O25(OH) V2O5 15 20 17 18 8 1000
Cr5B12O25(OH) Cr2O3; Cr(NO3)3·9 H2O 2; 1 0 6 0 9 1000
Mn5Mn0.83B12O26 Mn2O3 2.5 0 5 2 9 800
Mn5MnB12O22(OH)4 MnO 5 0 4 4 9 1200
Fe5Fe0.14B12O24.3(OH)1.7 Fe2O3 2.5 0 5 2 9 800

2.2 Phase identification and structure determination by X-ray diffraction

The products of the syntheses were large crystalline blocks of varying color, which formed together with one to three by-products. The crystalline products were thoroughly ground, mounted on a flat sample holder and analyzed by X-ray diffraction on a STOE Stadi P powder diffractometer. Measurements were performed in transmission geometry with Ge(111)-monochromatized MoK-L3 radiation (λ = 0.7093 Å) within a range of 2θ = 2–70°, a step size of 0.015° and a Mythen 1 K detector. The Topas 4.2 software [10] was used for the Rietveld refinement. One representative refinement is shown in Figure 3, the others are shown in the Supporting Information in Figures S1–S4.

Suitable crystals were isolated under a Leica 125M polarization microscope and measured with a Bruker D8 Quest diffractometer equipped with a Photon 300 CMOS detector. Multiscan absorption correction was performed with Sadabs-2016/2 [11]. The program suite WinGX-2018.1 [12] was used for the calculation of the structures, which were solved and refined with the implemented ShelXT-2018/2 [13] and ShelXL-2018/3 [14, 15] routines, respectively.

Further details of the crystal structure investigations may be obtained from the joint CCDC/FIZ Karlsruhe online deposition service: https://www.ccdc.cam.ac.uk/structures/? by quoting the deposition numbers CSD 2294261 for V5B12O25OH, CSD 2294262 for Cr5B12O25OH, CSD 2294263 for Mn5MnB12O22(OH)4, CSD 2294264 for Mn5Mn0.83B12O26, and CSD 2294265 for Fe5Fe0.14B12O24.3(OH)1.7.

2.3 Electron microprobe measurements

Single crystals of Mn5Mn0.83B12O26 and Fe5Fe0.14B12O24.3(OH)1.7 were investigated via electron microprobe measurements using a JEOL JXA-iSP100 Super Probe equipped with five WDS spectrometers and a fully integrated JEOL EDS system. The acceleration voltage used was 15 kV, with a beam current of 10 nA. To ensure electrical conductivity, a thin layer of carbon was deposited on the sample. The calibration samples used for the WDX measurement were magnetite (Fe3O4) and rhodonite (MnSiO3). K lines were used for the quantitative measurements.

3 Results and discussion

3.1 Experimental adaptations to unexpected findings

Initially, the aim of the conducted syntheses were the substances M5B12O25(OH) (M = V3+, Cr3+, Mn3+, Fe3+) from V2O5, Cr2O3/Cr(NO)3, Mn2O3, and Fe2O3 in combination with B2O3 and H3BO3. This targeted synthesis worked well for V5B12O25(OH) and Cr5B12O25(OH). However, the crystals of what was meant to be Mn5B12O25(OH) and Fe5B12O25(OH) immediately showed two issues that needed to be addressed: their cell volumes were too large when compared with the ionic radii of Mn3+ and Fe3+, and the significant residual electron density in the cuboctahedral cavities within the interpenetrating borate networks.

To investigate these unexpected findings, we conducted bond valence sum (BVS) calculations and performed electron microprobe measurements to rule out any contamination of the product with other elements and to detect a possible difference in composition.

One evidence is based on the M2–O distances, which are considerably longer than the corresponding M1–O distances, which results in a larger M2O6/M1O6 ratio (see Table 6). This is a strong indication that the octahedrally coordinated M2 position is occupied with a divalent metal cation instead of a trivalent one. On the other hand, the qualitative EDX measurements showed no other element than the respective metal, boron, and oxygen in the crystals, which means that the large cuboctahedral cavities have to be occupied by the comparably small transition metal cations. Based on these findings, we performed another synthesis with MnO as starting material This synthesis yielded the compound Mn5MnB12O22(OH)4, in which the cuboctahedral cavity is completely filled with Mn2+. The crystals are colorless in agreement with the oxidation state +2, while the crystals are brown when synthesized from Mn2O3.

The solid solution series with the end members MII5MIIB12O22(OH)4 and MIII5B12O25(OH) therefore represent the occupation of M sites with divalent and trivalent cations, respectively. The charge compensation of the anionic borate framework B12O26H x (16−x)− might vary, depending on the incorporated elements and their specific properties.

3.2 Powder X-ray diffraction and Rietveld refinements

Figure 4 shows a representative Rietveld refinement of Fe5Fe0.14B12O24.3(OH)1.7. The other Rietveld refinements are shown in the Supporting Information available online in Figures S1–S4. All occurring side products are listed in Table 2.

Figure 4: 
Rietveld refinement of Fe5Fe0.14B12O24.3(OH)1.7. The signal at 2θ = 8.2°, marked with an asterisk, stems from grease used to prepare a flat sample.
Figure 4:

Rietveld refinement of Fe5Fe0.14B12O24.3(OH)1.7. The signal at 2θ = 8.2°, marked with an asterisk, stems from grease used to prepare a flat sample.

Table 2:

Description of the products and side products. Tbp = “to be published”.

Product Side products
Figure 2 Substance Color Number Substance Color Reference
(a) V5B12O25(OH) Grayish-brown VBO3 Brown [16]
(b) Cr5B12O25(OH) Reddish-brown CrBO3 Green [17]
(c) Mn5MnB12O22(OH)4 Colorless MnB2O4 Brown [18]
(d) Mn5Mn0.83B12O26 Brownish-red 1 Mn4(B6O13(OH)) Red [19]
2 Mn3B7O13(BO4) Colorless Tbp
(e) Fe5Fe0.14B12O24.3(OH)1.7 Black 1 Fe2B3O7 Black [19]
2 Fe8B15O28(OH)8 Black [20]
3 Fe3B7O13(BO4) Colorless Tbp

3.3 Description of the products

Using the reaction conditions for the syntheses described above, most substances form large crystalline blocks of distinct color. This makes the separation from any side products relatively simple, except for Fe5Fe0.14B12O24.3(OH)1.7, for which two black side products are observed, which are known in the literature. Table 2 lists the color of the product and the side products of the syntheses; Figure 5 shows photographs of the samples. Some side products have not been known yet in the literature and will be reported elsewhere.

Figure 5: 
Photographs of the synthesized borates and their respective side products (Table 2). P = product, SP = side product.
Figure 5:

Photographs of the synthesized borates and their respective side products (Table 2). P = product, SP = side product.

3.4 Crystal structures

The five transition metal borates all crystallize in the space group I41/acd (no. 141), like all the known tetragonal representatives of this structure type [1], [2], [3]. One unit cell contains eight formula units (Z = 8). The lattice parameters vary between a = 1105.7–1178.98 pm and c = 2159.59–2217.46 pm, with a total cell volume V ranging from 2.6783 to 3.0823 nm3. In relation to their ionic radii, the cell volumes are in accordance with those of the published substances containing the interpenetrating (B12O26)16− networks, with the exception of Fe5Fe0.14B12O24.3(OH)1.7, which shows a larger cell volume than the ionic radius of iron would suggest. The two substances with the largest cell volumes, Mn5MnB12O25(OH) and Fe5Fe0.14B12O24.3(OH)1.7, exhibit a split position for the M2 cations. This phenomenon is also known in the literature for Ga5B12O25(OH) and In5B12O25(OH) [2]. The three substances that (partly) incorporate a cation in the cuboctahedral cavity, i.e. Fe5Fe0.14B12O24.3(OH)1.7, Mn5MnB12O22(OH)4, and Mn5Mn0.83B12O26, show a slightly larger a axis, as seen in Figure 6. Mn5MnB12O22(OH)4 and Mn5Mn0.83B12O26 also show a distinctly shortened c axis. This is due to the fact, that all three compounds feature the larger divalent cation rather than the trivalent cation on the M2 position. As the cuboctahedral cavity shows larger M3–O distances than the sum of the ionic radii of the respective cation and oxygen, the best structural refinements were achieved with a split position of the cation residing on M3.

Figure 6: 
Comparison of the cationic radii and the lattice parameters of the title compounds. Hollow dots are known from the literature, the full dots are from this publication. The trend line is calculated only from the literature-known values. Substances with different cations on the positions M1 and M2 are written as M1/M2.
Figure 6:

Comparison of the cationic radii and the lattice parameters of the title compounds. Hollow dots are known from the literature, the full dots are from this publication. The trend line is calculated only from the literature-known values. Substances with different cations on the positions M1 and M2 are written as M1/M2.

A list containing details of the structure refinements based on the single-crystal data is found in Table 3. Bond valence sums (BVS) were calculated for all substances with the bond-length/bond-strength concept [21, 22] and the charge distributions using the charge distribution in solids (CHARDI) concept [23, 24] are listed in Table 4. The interatomic distances are given in Table 5. Lists containing the atomic coordinates, thermal displacement factors and bond angles are given in the Supporting Information in Tables S1–S15.

Table 3:

Single-crystal data and structure refinement of M5B12O25(OH) (M = V3+, Cr3+), Mn5MnB12O22(OH)4, Mn5Mn0.83B12O26, and Fe5Fe0.14B12O24.3(OH)1.7.

Empirical formula V5B12O25(OH) Cr5B12O25(OH) Mn5MnB12O22(OH)4 Mn5Mn0.83B12O26 Fe5Fe0.14B12O24.3(OH)1.7
Molar mass, g mol−1 801.43 806.73 876.30 867.00 834.45
Crystal system Tetragonal
Space group I41/acd (no. 142)
Single-crystal diffractometer Bruker D8 Quest Kappa
Radiation/wavelength λ, Å MoK-L2,3/0.7107
a, pm 1118.58(1) 1105.70(5) 1179.0(2) 1141.47(5) 1135.57(1)
c, pm 2190.17(6) 2190.7(2) 2217.5(3) 2159.59(6) 2197.46(4)
V, nm3 2.7404(1) 2.6783(3) 3.082(8) 2.8138(2) 2.8337(1)
Formula units per cell Z 8 8 8 8 8
Calculated density, g cm−3 3.89 4.00 3.78 4.09 3.91
Crystal size, mm3 0.02 × 0.03 × 0.04 0.02 × 0.04 × 0.08 0.09 × 0.11 × 0.17 0.04 × 0.08 × 0.08 0.03 × 0.03 × 0.05
Temperature, K 173(2) 299(2) 301(2) 300(2) 301(2)
Absorption coefficient, mm−1 3.5 4.1 4.9 5.3 5.3
F(000), e 3072 3112 3365 3314 3227
θ range, deg 3.18–42.14 3.20–40.25 3.06–39.34 3.15–41.24 3.14–39.39
Range in hkl −21 ≤ h ≤ +20 −20 ≤ h ≤ +20 −21 ≤ h ≤ +21 −20 ≤ h ≤ +20 −20 ≤ h ≤ +18
−16 ≤ k ≤ +16 −20 ≤ k ≤ +20 −20 ≤ k ≤ +21 −20 ≤ k ≤ +20 −20 ≤ k ≤ +20
−28 ≤ l ≤ +41 −39 ≤ l ≤ +39 −39 ≤ l ≤ +39 −39 ≤ l ≤ +39 −39 ≤ l ≤ +39
Refl. total/independent 14147/2415 151893/2112 68847/2290 80042/2224 66815/2129
Rint/R σ 0.0440/0.0342 0.0448/0.0084 0.0442/0.0145 0.0558/0.0153 0.0703/0.0239
Refl. with I > 2 σ(I) 2023 2011 2200 2010 1776
Data/ref. parameters 2415/103 2112/103 2290/121 2224/109 2129/114
Absorption correction Multi-scan
Final R1/wR2 (I > 2 σ(I)) 0.0311/0.0753 0.0226/0.0571 0.0152/0.0373 0.0191/0.0457 0.0312/0.0754
Final R1/wR2 (all data) 0.0395/0.0804 0.0236/0.0576 0.0166/0.0377 0.0224/0.0472 0.0398/0.0799
Goodness-of-fit on F2 1.048 1.095 1.140 1.126 1.101
Largest diff. peak/hole, e Å−3 1.80/−1.30 1.62/−1.41 0.65/−0.73 0.62/−0.70 0.61/−1.37
Table 4:

Calculated charge distribution in M5B12O25(OH) (M = V3+, Cr3+), Mn5MnB12O22(OH)4, Mn5Mn0.83B12O26 and Fe5Fe0.14B12O24.3(OH)1.7 with the bond-length/bond-strength (ΣV) and the CHARDI (ΣQ) concept. For split positions with multiple sites, the charge of an atom in the center was calculated.

V1 V2 B1 B2 B3 H5 O1 O2 O3 O4 O5 O6 O7
ΣV 3.02 2.19 2.98 2.94 2.99 0.75 −1.98 −1.79 −1.86 −1.98 −1.99 −2.08 −1.70
ΣQ 2.98 2.97 3.01 3.04 2.97 1.01 −2.00 −1.92 −1.85 −1.99 −2.04 −2.12 −2.16
Cr1 Cr2 B1 B2 B3 H5 O1 O2 O3 O4 O5 O6 O7
ΣV 3.09 2.47 2.99 2.95 2.98 1.35 −1.99 −1.74 −1.92 −2.01 −2.22 −2.08 −1.66
ΣQ 2.99 2.99 3.00 3.04 2.97 1.01 −2.00 −1.92 −1.86 −2.01 −2.11 −2.11 −2.16
II Mn1 Mn2 Mn3 B1 B2 B3 H5 O1 O2 O3 O4 O5 O6 O7
ΣV 2.15 1.73 1.46 2.90 2.92 2.98 1.23 −1.78 −1.73 −1.82 −1.90 −2.18 −2.00 −1.92
ΣQ 1.96 1.87 2.00 3.04 3.13 2.99 0.93 −1.90 −1.79 −1.91 −1.88 −2.24 −2.14 −2.25
III Mn1 Mn2 Mn3 B1 B2 B3 O1 O2 O3 O4 O5 O6 O7
ΣV 2.93 1.95 1.69 3.00 2.93 2.97 −2.05 −1.88 −1.99 −2.07 −2.29 −2.20 −2.14
ΣQ 2.99 1.90 2.03 2.98 3.09 3.03 −1.98 −1.94 −1.89 −1.85 −2.08 −2.04 −2.31
Fe1 Fe2b Fe3 B1 B2 B3 H5 O1 O2 O3 O4 O5 O6 O7
ΣV 2.79 1.77 1.42 2.95 2.93 3.00 1.05 −1.93 −1.75 −1.82 −2.00 −2.02 −2.13 −1.94
ΣQ 2.97 1.98 1.82 3.00 3.05 2.96 1.02 −1.99 −1.88 −1.82 −2.04 −2.00 −2.21 −2.18
Table 5:

Selected interatomic distances and mean values (Å) in M5B12O25(OH) (M = V3+, Cr3+), Mn5MnB12O22(OH)4, Mn5Mn0.83B12O26, and Fe5Fe0.14B12O24.3(OH)1.7 (standard deviations in parentheses).

V5B12O25(OH) Cr5B12O25(OH) Mn5MnB12O22(OH)4 Mn5Mn0.83B12O26 Fe5Fe0.14B12O24.3(OH)1.7
M1– O6 1.9586(8) 1.9441(7) 2.1159(5) 1.9185(6) 1.964(2)
O5 1.9596(9) 1.9460(7) 2.1509(5) 1.8633(6) 2.015(2)
O3 2.0871(8) 2.0342(7) 2.2187(5) 2.1432(6) 2.112(2)
O4 1.9986(8) 1.9677(7) 2.1648(5) 2.0687(6) 2.005(2)
O5 1.9847(8) 1.9482(7) 2.2312(5) 2.0025(7) 2.089(2)
O1 2.0070(8) 1.9824(6) 2.3490(5) 2.1460(6) 2.093(2)
O4 2.5158(5)
av. M1–O 2.00 1.97 2.25 2.02 2.05
M2 O7 × 2 2.015(2) 2.0245(9) 2.0605(7) 2.0607(8)
O2 × 4 2.1794(8) 2.1056(6) 2.5705(5) 2.3091(6)
av. M2–O 2.12 2.08 2.40 2.23
M2b O7 × 2 2.1013(8) 2.061(2)
O2 × 2 2.345(2) 2.176(2)
O4 × 2 2.569(2)
O2 × 2 2.465(2)
av. M2b–O 2.34 2.23
M3 O6 × 4 2.5144(5) 2.6324(6) 2.605(2)
O1 × 4 2.5946(5) 2.4913(6) 2.594(2)
O4 × 4 2.7937(5) 2.5609(7) 2.636(2)
av. M3–O 2.63 2.56 2.61
B1– O1 1.476(2) 1.480(2) 1.4700(8) 1.479(2) 1.476(2)
O7 1.481(2) 1.466(2) 1.4709(7) 1.4274(9) 1.455(2)
O3 1.490(2) 1.480(2) 1.4810(8) 1.469(2) 1.485(2)
O4 1.475(2) 1.490(2) 1.5262(8) 1.532(2) 1.509(2)
av. B1–O 1.48 1.48 1.49 1.48 1.48
B2– O3 1.499(2) 1.498(2) 1.4792(8) 1.477(2) 1.506(2)
O2 1.487(2) 1.490(2) 1.4827(7) 1.454(2) 1.475(2)
O6 1.472(2) 1.469(2) 1.4845(8) 1.524(2) 1.476(2)
O1 1.483(2) 1.477(2) 1.4925(8) 1.479(2) 1.478(2)
av. B2–O 1.49 1.48 1.48 1.48 1.48
B3– O6 1.473(2) 1.473(2) 1.4620(8) 1.521(2) 1.466(2)
O5 1.456(2) 1.458(2) 1.4814(8) 1.467(2) 1.495(2)
O2 1.514(2) 1.525(2) 1.4815(8) 1.448(2) 1.475(2)
O4 1.473(2) 1.467(2) 1.4821(8) 1.483(2) 1.466(2)
av. B3–O 1.48 1.48 1.48 1.48 1.48
  1. The bold values represent the averages.

The discrepancy of the calculated BVS with the formal oxidation numbers for the M2 position is due to the longer M2–O distances compared to M1–O distances, which are very close the formal oxidation number, as both positions contain the same cation and are octahedrally coordinated. This variation on size of the octahedra is intrinsic to this structure type; hence, most BVS calculations yield a lower charge for the M2 position, when both positions are occupied with the same cation. One exception is Ga4InB12O25(OH), as in this case the appropriately larger cation occupies the larger octahedron [3]. For all substances with mixed valency, we therefore conclude that the cation with the higher oxidation number is found in the M1 octahedra, in contrast to the first publication on this field, which stated that Ti4+ was on the M2 position [1].

To compare the different substances, we analyzed the volume of the coordination polyhedra. It can be seen that the volume of the cuboctahedron relative to that of the octahedra decreases with the increasing occupancy of the central cation position. This makes sense, as the cation reduces the Coulomb repulsion between the vertices of the polyhedron. Furthermore, the volume of the M2O6 octahedra is larger when occupied with a divalent rather than a trivalent cation. These values and trends can be observed in Table 6. Based on the size of the Fe1O6 octahedron and the ”higher than expected” cell volume we conclude that it hosts both: the larger Fe2+ and smaller Fe3+ cations, either in different domains of the single crystal or as a part of a solid solution series between M5B12O25(OH) and M5MB12O22(OH)4.

Table 6:

Volume of the octahedral (M1O6, M2O6) and cuboctahedral cavities and of the cuboctahedrally coordinated cations M3 (M3O12) of all substances. The ratio of M1O6 to the other polyhedra is also given.

V3+ Cr3+ Mn2+ Mn3+/2+ Fe3+/2+
M1O6 10.58 10.15 13.41 10.82 11.24
M2O6 12.60 11.85 17.45 14.32 14.40
M3O12 40.71 40.03 43.22 39.75 41.75
M2O6/M1O6 1.19 1.17 1.30 1.32 1.28
M3O12/M1O6 3.85 3.94 3.22 3.67 3.71
Occupancy M3O12, % 0 0 100 83 14

3.5 Electron microprobe measurements

To rule out the contamination with another element, single crystals of Fe5Fe0.14B12O24.3(OH)1.7 and Mn5Mn0.83B12O26 were analyzed quantitatively with WDX and qualitatively and semiquantitatively with EDX. No other elements than B, O, and the respective metal could be detected. The standards used for calibration were natural minerals: Fe3O4 and MnSiO3. Due to the lack of reference materials for B and O, these elements were added as fixed, based on the expected composition of the sample to ensure proper matrix correction. Representative EDX spectra for both substances are depicted in Figure 7. Figure 8 shows BSE pictures of the samples, with an overview in (a) and (c) and a focus on crystals, which appeared to be single-crystalline in (b) and (d). In fact, several crystal domains can be seen; the difference in color indicates a variation in the metal to borate ratio. These ratios all fall within the solid solution series M6B12O22(OH)4 – M5B12O25(OH) when factoring in the error of the measurements, which are the combination of using different calibration compounds (up to ∼1 % w/w) and the standard deviation of results. Hence, these results offer an explanation for the partial occupation of the cuboctahedral cavities. Table 7 lists the averaged results of the quantitative WDX measurements, as well as the minimum and maximum value measured for the specific metal and the respective standard deviation of the results.

Figure 7: 
EDX spectra of Mn5Mn0.83B12O26 (top) and Fe5Fe0.14B12O24.3(OH)1.7 (bottom).
Figure 7:

EDX spectra of Mn5Mn0.83B12O26 (top) and Fe5Fe0.14B12O24.3(OH)1.7 (bottom).

Figure 8: 
BSE pictures of Mn5Mn0.83B12O26 (a, b) and Fe5Fe0.14B12O24.3(OH)1.7 (c, d).
Figure 8:

BSE pictures of Mn5Mn0.83B12O26 (a, b) and Fe5Fe0.14B12O24.3(OH)1.7 (c, d).

Table 7:

Quantitative WDX measurements of Mn5Mn0.83B12O26 and Fe5Fe0.14B12O24.3(OH)1.7. The detected minimum, maximum, average and theoretical values for the metals are given.

Element (%; w/w)
Element Min Max Average Std. deviation Theoretical
Mn 38.1 39.0 38.5 0.9 37.0
Fe 33.4 36.7 34.8 1.8 34.4
  1. The bold values represent the averages.

We hence conclude that the crystals in the systems Mn–B–O(–H) and Fe–B–O–H in fact show several domains of the solid solution series between completely divalent and trivalent metal cations. In the case of the iron compound, the protonation and occupation of the cuboctahedral M3O12 site within the FBBs plays a role, whereas the needed charge compensation in the manganese containing compound is primarily achieved by filling the M3O12 site with the metal cation.

4 Conclusions

In this publication, we present several new representatives of the Ga5B12O25(OH) structure type, as well as an adaptation of the structure type to incorporate divalent instead of trivalent cations. Charge compensation is then achieved by incorporation of more hydrogen atoms and by the occupation of the hitherto unoccupied cuboctahedral cavity, which shows rather large M–O distances with the comparable small transition metal cation. The early transition metals V and Cr are completely trivalent and form structures isotypic to Ga5B12O25(OH). Mn and Fe are partially reduced to the oxidation state +2 and hence can enter the larger cuboctahedral cavities. With the use of MnO as starting material it is possible to achieve the compound Mn5MnB12O22(OH)4 with all Mn atoms in the divalent state. These findings are backed by single-crystal X-ray diffraction and electron microprobe measurements, through which any contamination with other elements could be ruled out. Furthermore, the formation of domains with different metal contents and therefore different oxidation states of the cations could be identified within the single crystals on the BSE pictures, which offer the explanation for the odd occupancy of the cuboctahedral cavity that appeared during the structure refinement via single-crystal X-ray diffraction data. This conclusion also explains the too large cell volume of Fe5Fe0.14B12O24.3(OH)1.7. This is the first paper of a series, which features the structural diversity of this anionic borate network as a host for a manifold of cations. Different combinations of cations within the same environment appear to be suitable targets for further systematic synthetic and spectroscopic investigations.

5 Supporting information

The Rietveld refinements of all substances not shown in the main text and additional crystal structure data are given as supplementary material available online (https://doi.org/10.1515/znb-2023-0082).


Dedicated to Professor Wolfgang Bensch on the occasion of his 70th birthday.



Corresponding author: Hubert Huppertz, Department of General, Inorganic and Theoretical Chemistry, University of Innsbruck, Innrain 80–82, 6020 Innsbruck, Austria, E-mail:

Acknowledgments

We thank Ass.-Prof. Dr. Klaus Wurst and Assoc.-Prof. Dr. Gunter Heymann for the recording of the single-crystal data. LCP is grateful for the PhD scholarship of the University of Innsbruck.

  1. Research ethics: Not applicable.

  2. Author contributions: The authors have accepted responsibility for the entire content of this manuscript and approved its submission.

  3. Competing interests: The authors state no conflict of interest.

  4. Research funding: None declared.

  5. Data availability: The raw data can be obtained on request from the corresponding author.

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Supplementary Material

This article contains supplementary material (https://doi.org/10.1515/znb-2023-0082).


Received: 2023-09-16
Accepted: 2023-09-30
Published Online: 2024-01-12
Published in Print: 2024-01-29

© 2023 the author(s), published by De Gruyter, Berlin/Boston

This work is licensed under the Creative Commons Attribution 4.0 International License.

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